Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
| Beide Seiten der vorigen RevisionVorhergehende ÜberarbeitungNächste Überarbeitung | Vorhergehende Überarbeitung | ||
| en:berechnungen:festigkeitsberechnung [2025/02/24 10:46] – [Shear Stress] cschall | en:berechnungen:festigkeitsberechnung [2025/09/03 12:27] (aktuell) – [Shear Stress] neelest | ||
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| Zeile 1: | Zeile 1: | ||
| ======Stress Analysis====== | ======Stress Analysis====== | ||
| - | -> [[grafische_darstellung_der_ergebnisse: | + | -> [[..:grafische_darstellung_der_ergebnisse: |
| ===== Equivalent Stress===== | ===== Equivalent Stress===== | ||
| Zeile 9: | Zeile 9: | ||
| $$σ_v = \sqrt {(σ_x - σ_y)^2 + 4τ_{xy}^2}$$ | $$σ_v = \sqrt {(σ_x - σ_y)^2 + 4τ_{xy}^2}$$ | ||
| - | Since the rotation of the screw is purely | + | Since the rotation of the screw represents a purely |
| + | As bending of the screw can also be neglected, the normal stress in the y-direction | ||
| + | $\sigma_y$ may likewise | ||
| + | The normal stress in the x-direction | ||
| $$σ_v = \sqrt {σ_x^2 + 4τ_{xy}^2}$$ | $$σ_v = \sqrt {σ_x^2 + 4τ_{xy}^2}$$ | ||
| Zeile 32: | Zeile 35: | ||
| The shear stress resulting from the applied torque is calculated using the following formula: | The shear stress resulting from the applied torque is calculated using the following formula: | ||
| - | $$\tau_{nenn} = \frac{M_t}{W_t} = \frac{M_t \cdot a_{max}}{I_p}$$ | + | $$\tau_{nominal} = \frac{M_t}{W_t} = \frac{M_t \cdot a_{max}}{I_p}$$ |
| with the torque $M_t$, the section modulus $W_t$, the polar moment of inertia $I_p$ and the maximum perpendicular distance from the outer fiber to the neutral (stress-free) fiber $a_{max}$. | with the torque $M_t$, the section modulus $W_t$, the polar moment of inertia $I_p$ and the maximum perpendicular distance from the outer fiber to the neutral (stress-free) fiber $a_{max}$. | ||
| - | Another influencing factor for calculating the worm gear strength is the radius that describes the transition from the worm root to the web. For this geometric influence, a shape factor (stepped round bar under torsion, DIN 743-2) is defined as: | + | Another influencing factor for calculating the screw strength is the radius that describes the transition from the screw core to the flight. For this geometric influence, a shape factor (stepped round bar under torsion, DIN 743-2) is defined as: |
| $$\alpha_{\tau} = 1+ \frac{1}{\sqrt{3, | $$\alpha_{\tau} = 1+ \frac{1}{\sqrt{3, | ||
| Zeile 45: | Zeile 48: | ||
| $$\beta_{\tau} = \frac{\alpha_\tau}{n}$$ | $$\beta_{\tau} = \frac{\alpha_\tau}{n}$$ | ||
| - | $$\text{mit}$$ | + | $$\text{with}$$ |
| $$n=1+\sqrt{G' | $$n=1+\sqrt{G' | ||
| - | $$\text{und}$$ | + | $$\text{and}$$ |
| $$G' | $$G' | ||
| Zeile 54: | Zeile 57: | ||
| $$K_\tau = \left( \frac{\beta_\tau}{K_2(d)}+\frac{1}{K_{F, | $$K_\tau = \left( \frac{\beta_\tau}{K_2(d)}+\frac{1}{K_{F, | ||
| $$\text{with}$$ | $$\text{with}$$ | ||
| - | $$K_2(d)=1-0, | + | $$K_2(d)=1-0, |
| - | with the influence of the surface roughness $K_{F, | + | as well as with the influence of surface roughness $K_{F, |
| + | The values apply up to a diameter of 25 mm and decrease linearly beyond this value down to 1.0 at a diameter of 40 mm. For diameters above 40 mm, the value remains constant at 1.0. | ||
| - | Finally, the shear stress, taking | + | The resulting |
| - | $$\tau_{xy} = \tau_{max}=\tau_{nenn} \cdot K_\tau$$ | + | $$\tau_{xy} = \tau_{max}=\tau_{nominal} \cdot K_\tau$$ |
| ===Further topics=== | ===Further topics=== | ||
| * [[en: | * [[en: | ||
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